Transactions of the Cambridge Philosophical Society, المجلد 22University Press, 1923 |
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الصفحة
... Transformation of Differential Operators which present themselves in Invariant Theories . By Major P. A. MACMAHON , F.R.S. VIII . Vector Integral Equations and Gibbs ' Dyadics . By C. E. WEATHERBURN , Ormond College , University of ...
... Transformation of Differential Operators which present themselves in Invariant Theories . By Major P. A. MACMAHON , F.R.S. VIII . Vector Integral Equations and Gibbs ' Dyadics . By C. E. WEATHERBURN , Ormond College , University of ...
الصفحة 23
... transformation which is sug- gested by the work in that part of Barnes ' memoir on integral functions which deals with the generalised function of Mittag - Leffler : Ea ( x ; 0 , B ) = ± Σ n = 0 xn [ ( 1 + an ) . ( n + H ) B · The ...
... transformation which is sug- gested by the work in that part of Barnes ' memoir on integral functions which deals with the generalised function of Mittag - Leffler : Ea ( x ; 0 , B ) = ± Σ n = 0 xn [ ( 1 + an ) . ( n + H ) B · The ...
الصفحة 40
... transformed the equation V1 = 0 , which is satisfied by the stream function , from Cartesian coordinates ( x , y ) to ... transformation is to introduce relatively unimportant terms , as will be seen below . The coordinate a will be ...
... transformed the equation V1 = 0 , which is satisfied by the stream function , from Cartesian coordinates ( x , y ) to ... transformation is to introduce relatively unimportant terms , as will be seen below . The coordinate a will be ...
الصفحة 77
... transformed curve approaches P touching the line 70 but above it as shewn by terms of the next order . On this transformed boundary r ' is not zero for the motion in which the least axis is that of rotation . The region SHP represents ...
... transformed curve approaches P touching the line 70 but above it as shewn by terms of the next order . On this transformed boundary r ' is not zero for the motion in which the least axis is that of rotation . The region SHP represents ...
الصفحة 99
... TRANSFORMATION OF DIFFERENTIAL OPERATORS WHICH PRESENT THEMSELVES IN INVARIANT THEORIES BY MAJOR P. A. MACMAHON , F.R.S. HONORARY MEMBER OF THE CAMBRIDGE PHILOSOPHICAL SOCIETY . CAMBRIDGE : AT THE UNIVERSITY PRESS M.DCCCC . XV ...
... TRANSFORMATION OF DIFFERENTIAL OPERATORS WHICH PRESENT THEMSELVES IN INVARIANT THEORIES BY MAJOR P. A. MACMAHON , F.R.S. HONORARY MEMBER OF THE CAMBRIDGE PHILOSOPHICAL SOCIETY . CAMBRIDGE : AT THE UNIVERSITY PRESS M.DCCCC . XV ...
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a₁ angle approximately asymptotic expansion atmosphere Axiom of Archimedes axis b₁ c₁ calculated coefficients considered constant convergent convex set cordon corresponding cos² curve d₁ definition denote density determined differential equations disturbance diurnal diurnal variations dyadic earth equal escape expression factor finite follows formula free path function G. H. Hardy giant star given h₂ Hence integral equation invariant Jacobian k₁ k₂ magnitude molecules obtained orbit paper parameters partitions plane positive potential Primitive Roots ratio relation respectively result rotation scalar shew shewn sin² solar solid angle solutions substitution suppose surface t₁ theorem theory v₁ values vector velocity w₁ X₁ XXII zero Σ Σ дх